A differential input circuit (1-1) includes first (Q0) and second (Q1) input transistors having control electrodes coupled to first (Vin+) and second (Vin−) input signals, respectively. A pass transistor (P3) is coupled between first electrodes of the first and second input transistors. first (N1) and second (N2) level shift transistors have control electrodes coupled to the first and second input signals, respectively. A voltage selector circuit (22) selects a voltage on a first electrode of one of the first and second level shift transistors according to which is at a higher voltage, and produces a corresponding control voltage (V19) on a control electrode of the pass transistor so as to limit a voltage difference between the first electrode and the control electrode of the first input transistor (Q0) when it is turned off in response to a large difference between the first and second input signals.
|
20. A differential input circuit comprising:
(a) first and second input transistors each having a first electrode, a second electrode, and a control electrode, the differential input circuit also including circuitry for biasing the first and second input transistors, the control electrode of the first input transistor being coupled to a first input signal, and the control electrode of the second input transistor being coupled to a second input signal;
(b) a pass transistor coupled between the first electrode of the first input transistor and the first electrode of the second input transistor for limiting the voltage difference between the first electrode and the control electrode of the first input transistor when it is turned off in response to a large difference between the first and second input signals, the pass transistor being a jfet (junction field effect transistor);
(c) means for operating a level shift transistor in response to the first input signal to produce a first signal on a first electrode of a first voltage selector transistor so as to forward bias a pn junction of the first voltage selector transistor and thereby produce a second signal on a gate of the first voltage selector transistor if the magnitude of a predetermined one of the first and second input signals substantially exceeds the magnitude of the other; and
(d) means for causing the second signal to be applied to a gate of the pass transistor so as to produce a third signal on both a source of the pass transistor and the first electrode of the first input transistor so that the third signal follows the first input signal and limits a voltage difference between the first electrode and the control electrode of the first input transistor if the magnitude of the predetermined one of first and second input signals substantially exceeds the magnitude of the other.
15. A method for operating a differential input circuit including
1) first and second input transistors each having a first electrode, a second electrode, and a control electrode, the differential input circuit also including circuitry for biasing the first and second input transistors, the control electrode of the first input transistor being coupled to a first input signal, and the control electrode of the second input transistor being coupled to a second input signal, and
2) a pass transistor coupled between the first electrode of the first input transistor and the first electrode of the second input transistor for limiting a voltage difference between the first electrode and the control electrode of the first input transistor when it is turned off in response to a large difference between the first and second input signals, the pass transistor being a fet (field effect transistor),
the method comprising:
(a) operating a level shift transistor in response to the first input signal to produce a first signal on a first electrode of a first voltage selector transistor so as to forward bias a pn junction of the first voltage selector transistor and thereby produce a second signal on a gate of the first voltage selector transistor if the magnitude of a predetermined one of the first and second input signals substantially exceeds the magnitude of the other; and
(b) applying the second signal to a gate of the pass transistor so as to cause it to produce a third signal on both a source electrode of the pass transistor and the first electrode of the first input transistor so that the third signal follows the first input signal and thereby limits a voltage difference between the first electrode and the control electrode of the first input transistor if the magnitude of the predetermined one of the first and second input signals substantially exceeds the magnitude of the other.
1. A differential input circuit comprising:
(a) first and second input transistors each having a first electrode, a second electrode, and a control electrode, the control electrode of the first input transistor being coupled to a first input signal, and the control electrode of the second input transistor being coupled to a second input signal, and circuitry for biasing the first and second input transistors;
(b) a pass transistor coupled between the first electrode of the first input transistor and the first electrode of the second input transistor, for limiting a voltage difference between the first electrode and the control electrode of the first input transistor when it is turned off in response to a large difference between the first and second input signals, the pass transistor being a fet (field effect transistor); and
(c) clamping circuitry coupled to the first and second input signals and also coupled to a control electrode of the pass transistor for controlling the pass transistor, the clamping circuitry including
1) a first level shift transistor having a first electrode, a second electrode, and a control electrode, and a second level shift transistor having a first electrode, a second electrode, and control electrode, the first electrodes of the first and second level shift transistors being coupled to a first supply voltage, the control electrodes of the first and second level shift transistors being coupled to the first and second input signals, respectively, and
2) a voltage selector circuit coupled between the second electrodes of the first and second level shift transistors for selecting a voltage on the second electrode of one of the first and second level shift transistors according to which of the second electrodes of the first and second level shift transistors is at a higher voltage, and producing a corresponding control voltage on the control electrode of the pass transistor.
2. The differential input circuit of
3. The differential input circuit of
4. The differential input circuit of
5. The differential input circuit of
6. The differential input circuit of
7. The differential input circuit of
8. The differential input circuit of
9. The differential input circuit of
10. The differential input circuit of
11. The differential input circuit of
12. The differential input circuit of
13. The differential input circuit of
14. The differential input circuit of
16. The method of
17. The method of
18. The method of
19. The method of
|
The present invention relates generally to improving reliability of differentially coupled input transistors of a comparator or amplifier, and more particularly to preventing damage caused by hot carrier injection (HCI), and especially to preventing HCI due to excessive reverse bias of base-emitter junctions of differentially coupled input transistors of the comparator or amplifier or excessive gate-source voltages of differentially coupled field effect input transistors of the comparator or amplifier.
A comparator is a circuit that determines whether its input signal is higher (or lower) than a fixed or varying reference signal and accordingly switches its output to a high (or low) logic level. A comparator need not be as multi-functional as an operational amplifier, but a comparator needs to respond faster than an operational amplifier, and do so with a smaller magnitude input overdrive voltage (i.e., with a smaller difference between the input voltage to one input of the comparator and a reference voltage applied to the other input of the comparator). For a comparator, this is an advantage because phase margin and unity gain stability are not of primary concern. A basic specification for a comparator is its comparator delay TDELAY, which is the time required for the comparator output to switch after detecting its minimum input overdrive voltage. Another specification is input overdrive voltage VOVDR, which is the minimum differential input voltage at which the comparator responds by switching its output signal. The minimum small signal gain of a comparator can be roughly calculated as VSUPPLY/VOVDR (input overdrive voltage). In order to achieve this gain at the necessary speed, at least two gain stages typically are required.
One of the important considerations of comparator design is the reliability of its input transistors. If a large signal differential voltage, e.g., greater than 2 volts, is applied at the inputs of a typical differential input transistor pair, the input transistor that is in its OFF or “cut-off” condition experiences a large emitter-base junction reverse bias voltage VEBO that exceeds 0.7 volt. This causes hot carrier generation (e.g., a tunneling or avalanche effect) in the base-emitter junction of that input transistor and may permanently degrade the current gain β and performance of the input transistor.
Prior Art
This is especially true for modern wafer fabrication processes in which such hot electron injection is very likely to degrade the current gain β and hence the performance of the input transistors over time. (It is believed that injected high-energy or “hot” electrons become trapped in the emitter-base junction and thereby cause the above mentioned degradation of the β of the transistor.) This can cause the matching of input transistors Q0 and Q1 to change over time due to the effects of the above mentioned large reverse bias. That would result in permanent changing over time of the input offset voltage Vos of the differential input stage. That would be highly undesirable because it would cause the switching point of a comparator to change over time.
Similarly, if MOS input transistors are used instead of PNP input transistors Q0 and Q1, a similar large gate-source reverse bias voltage on the “cut-off” MOS input transistor can result in hot electron injection that may cause a shift in the turn-on threshold voltage VT of that input transistor. Differentially coupled JFET input transistors also may undergo undesirable permanent changes due to hot electron injection.
To overcome the hot electron injection problem described above, some comparators of the prior art use a CMOS input stage which can tolerate large reverse bias between the gate and source electrodes of an input transistor. Some previous comparators include differentially coupled bipolar input transistors that can tolerate large reverse bias across their emitter-base junctions. However, as device sizes have become smaller, transistors fabricated using some recent bipolar integrated circuit manufacturing processes do not have the ability to tolerate such large reverse bias across their base-emitter junctions, and a solution to the above mentioned hot electron injection problem is needed more than ever. Up to now, the hot electron injection problem in comparator input stages has been avoided mainly by using older wafer fabrication processes to fabricate bipolar transistors that are capable of withstanding the large emitter-base reverse bias voltages.
The closest prior art is also believed to include commonly owned U.S. Pat. No. 7,339,402 entitled “Differential Amplifier with Overvoltage Protection and Method” issued Mar. 4, 2008 to Alenin et al. Prior Art
Thus, there is an unmet need for a differential input stage of a comparator or amplifier to prevent circuit degradation due to hot carrier injection resulting from large differential input voltages.
There also is an unmet need for a differential input stage of a comparator or amplifier to prevent circuit degradation due to hot carrier injection across the emitter-base junction of a bipolar (PNP or NPN) input transistor of the differential input stage resulting from large differential input voltages applied to the differential input stage.
There also is an unmet need for a differential input stage for a comparator or amplifier which prevents circuit degradation due to hot carrier injection in a field effect input transistor of the differential input stage resulting from large differential input voltages applied to the differential input stage.
There also is an unmet need for a differential input stage for a comparator or amplifier which is able to prevent reverse bias voltages that are sufficiently large to damage the input transistors, without causing large input currents, without large internal quiescent currents, and which allows the common mode voltage or the supply voltage of the comparator or amplifier to operate beyond maximum voltage levels that can be tolerated by unprotected input transistors.
It is an object of the invention to provide a differential input stage for a comparator or amplifier to prevent circuit degradation due to hot carrier injection resulting from large differential input voltages.
It is another object of the invention to provide a differential input stage for a comparator or amplifier to prevent circuit degradation due to hot carrier injection across the emitter-base junction of a bipolar (PNP or NPN) input transistor of the differential input stage resulting from large differential input voltages applied to the differential input stage.
It is another object of the invention to provide a differential input stage for a comparator or amplifier which prevents circuit degradation due to hot carrier injection in a field effect input transistor of the differential input stage resulting from large differential input voltages applied to the differential input stage.
It is another object of the invention to provide a differential input stage for a comparator or amplifier which is able to prevent sufficiently large reverse bias voltages of input transistors from damaging them, without causing large input currents, without large internal quiescent currents, and without requiring the common mode voltage or the supply voltage of the comparator or amplifier to operate beyond maximum voltage levels that can be tolerated by an unprotected input transistors.
Briefly described, and in accordance with one embodiment, the present invention provides a differential input circuit (1-1) includes first (Q0) and second (Q1) input transistors having control electrodes coupled to first (Vin+) and second (Vin−) input signals, respectively. A pass transistor (P3) is coupled between first electrodes of the first and second input transistors. First (N1) and second (N2) level shift transistors have control electrodes coupled to the first and second input signals, respectively. A voltage selector circuit (22) selects a voltage on a first electrode of one of the first and second level shift transistors according to which is at a higher voltage, and produces a corresponding control voltage (V19) on a control electrode of the pass transistor so as to limit a voltage difference between the first electrode and the control electrode of the first input transistor (Q0) when it is turned off in response to a large difference between the first and second input signals.
In one embodiment, the invention provides a differential input circuit (1-1) including first (Q0) and second (Q1) input transistors each having a first electrode, a second electrode, and a control electrode, the control electrode of the first input transistor (Q0) being coupled to a first input signal (Vin+), and the control electrode of the second input transistor (Q1) being coupled to a second input signal (Vin−), and circuitry (I0,I5) for biasing the first (Q0) and second (Q1) input transistors. A pass transistor (P3) is coupled between the first electrode (11A) of the first input transistor (Q0) and the first electrode (11B) of the second input transistor (Q1), for limiting a voltage difference between the first electrode and the control electrode of the first input transistor (Q0) when it is turned off in response to a large difference (Vin+−Vin−) between the first (Vin+) and second (Vin−) input signals, the pass transistor (P3) being a FET (field effect transistor). Clamping circuitry (14) is coupled to the first (Vin+) and second (Vin−) input signals and is also coupled to a control electrode of the pass transistor (P3) for controlling the pass transistor (P3). The clamping circuitry includes a first level shift transistor (N1) having a first electrode, a second electrode, and a control electrode, and a second level shift transistor (N2) having a first electrode, a second electrode, and control electrode, the first electrodes of the first (N1) and second (N2) level shift transistors being coupled to a first supply voltage (VCC), the control electrodes of the first (N1) and second (N2) level shift transistors being coupled to the first (Vin+) and second (Vin−) input signals, respectively. The clamping circuitry also includes a voltage selector circuit (22 or 22A) coupled between the second electrodes of the first (N1) and second (N2) level shift transistors for selecting a voltage on the second electrode of one of the first (N1) and second (N2) level shift transistors according to which of the second electrodes of the first (N1) and second (N2) level shift transistors is at a higher voltage, and producing a corresponding control voltage on the control electrode of the pass transistor (P3).
In one embodiment, the voltage selector circuit (22 in
A described embodiment, the biasing circuitry includes first (I0) and second (I5) current sources coupled to the first electrodes of the first (Q0) and second (Q1) input transistors, respectively, the differential input circuit also including fifth (I2) and sixth (I3) current sources coupled to bias the first (N1) and second (N2) level shift transistors, respectively. The first (Q0) and second (Q1) input transistors may be PNP transistors. The pass transistor (P3) may be a P-channel JFET (junction field effect transistor). The first (P1) and second (P2) voltage selector transistors may be P-channel JFETs. The first (N1) and second (N2) level shift transistors may be N-channel JFETs. In one embodiment, the first (PNP1 in
In one embodiment, the differential input circuit includes a first follower circuit (30 in
In one embodiment, a source-gate junction of the first voltage selector transistor (P1) is forward biased when the first input signal (Vin+) is substantially greater than the second input signal (Vin−).
In one embodiment, the invention provides a method for operating a differential input circuit (1-1) that includes first (Q0) and second (Q1) input transistors each having a first electrode, a second electrode, and a control electrode, the differential input circuit (1-1) also including circuitry (I0,I5) for biasing the first (Q0) and second (Q1) input transistors, the control electrode of the first input transistor (Q0) being coupled to a first input signal (Vin+), and the control electrode of the second input transistor (Q1) being coupled to a second input signal (Vin−), and a pass transistor (P3) coupled between the first electrode (11A) of the first input transistor (Q0) and the first electrode (11B) of the second input transistor (Q1) for limiting a voltage difference between the first electrode and the control electrode of the first input transistor (Q0) when it is turned off in response to a large difference (Vin+−Vin−) between the first (Vin+) and second (Vin−) input signals, the pass transistor (P3) being a FET (field effect transistor), the method including operating a level shift transistor (N1) in response to the first input signal (Vin+) to produce a first signal (V20) on a first electrode of a first voltage selector transistor (P1) so as to forward bias a PN junction of the first voltage selector transistor (P1) and thereby produce a second signal (V19) on a gate of the first voltage selector transistor (P1) if the magnitude of a predetermined one of the first (Vin+) and second (Vin−) input signals substantially exceeds the magnitude of the other; and applying the second signal (V19) to a gate of the pass transistor (P3) so as to cause it to produce a third signal (V11A) on both a source electrode of the pass transistor (P3) and the first electrode (11A) of the first input transistor (Q0) so that the third signal (V11A) follows the first input signal (Vin+) and thereby limits a voltage difference between the first electrode (11A) and the control electrode of the first input transistor (Q0) if the magnitude of the predetermined one of the first (Vin+) and second (Vin−) input signals substantially exceeds the magnitude of the other.
In one embodiment, the method includes biasing the first (Q0) and second (Q1) input transistors by means of first (I0) and second (I5) current sources coupled to the first electrodes of the first (Q0) and second (Q1) input transistors, respectively, and biasing the first level shift transistor (N1) by means of a third current source (I2). In one embodiment, the level shift transistor (N1) is a junction field effect transistor, and the method includes forward-biasing a gate-source junction of the level shift transistor (N1) when the first input signal (Vin+) is substantially greater than the second input signal (Vin−).
In one embodiment, the method includes providing a follower circuit (30) having an input coupled to the first input signal (Vin+) and an output (23) coupled the control electrodes of the level shift transistor (N1) and the first input transistor (Q0), and wherein the follower circuit (30) includes a follower transistor (Q3) having a control electrode coupled to the first input signal (Vin+) and a first electrode (23) coupled to the control electrode of the level shift transistor (N1), the method including shifting the level of the first signal (V20) by means of a level shift resistor (R0) coupled between the control electrode (26) of the first input transistor (Q0) and the control electrode of the level shift transistor (N1). In one embodiment, the first (Q0) and second (Q1) input transistors are PNP transistors and the method includes limiting reverse bias voltages across an emitter-base junction of the first input transistor (Q0) to approximately 2 volts.
In one embodiment, the invention provides a differential input circuit (1-1) including first (Q0) and second (Q1) input transistors each having a first electrode, a second electrode, and a control electrode, the differential input circuit (1-1) also including circuitry (I0,I5) for biasing the first (Q0) and second (Q1) input transistors, the control electrode of the first input transistor (Q0) being coupled to a first input signal (Vin+), and the control electrode of the second input transistor (Q1) being coupled to a second input signal (Vin−); a pass transistor (P3) coupled between the first electrode (11A) of the first input transistor (Q0) and the first electrode (11B) of the second input transistor (Q1) for limiting the voltage difference between the first electrode and the control electrode of the first input transistor (Q0) when it is turned off in response to a large difference (Vin+−Vin−) between the first (Vin+) and second (Vin−) input signals, the pass transistor (P3) being a JFET (junction field effect transistor); means (15, I2) for operating a level shift transistor (N1) in response to the first input signal (Vin+) to produce a first signal (V20) on a first electrode of a first voltage selector transistor (P1) so as to forward bias a PN junction of the first voltage selector transistor (P1) and thereby produce a second signal (V19) on a gate of the first voltage selector transistor (P1) if the magnitude of a predetermined one of the first (Vin+) and second (Vin−) input signals substantially exceeds the magnitude of the other; and means (14) for causing the second signal (V19) to be applied to a gate of the pass transistor (P3) so as to produce a third signal (V11A) on both a source of the pass transistor (P3) and the first electrode (11A) of the first input transistor (Q0) so that the third signal (V11A) follows the first input signal (Vin+) and limits a voltage difference between the first electrode (11A) and the control electrode of the first input transistor (Q0) if the magnitude of the predetermined one of first (Vin+) and second (Vin−) input signals substantially exceeds the magnitude of the other.
The present invention solves the above mentioned problems associated with HCI (hot carrier injection) due to large differential input voltages of a comparator or amplifier input stage, by clamping the base-emitter junction of emitter-coupled input transistors so as to limit the amount of reverse bias of the emitter-base junctions and thereby prevent HCI.
As previously indicated, one of the important considerations in the design of input stages for comparators and some amplifiers is the reliability of the input transistors. If a large signal differential input voltage VD(max) of magnitude greater than approximately 2 volts is applied at the inputs of a pair of typical differentially-coupled input transistors, one of the input transistors is turned ON and the other is turned completely OFF, i.e. is “cut off”. The cut off transistor undergoes a large emitter-base reverse bias voltage VEBO greater than approximately 0.7 volt. The large reverse breakdown voltage causes generation of hot (i.e., high energy) carriers (predominantly due to tunneling effects in some modern wafer fabrication processes) in the base-emitter junction of the cut off input transistor, and the resulting hot carrier injection may permanently degrade the performance of that input transistor.
In
Similarly, input stage 1-1 includes a PNP input transistor Q1 having its base connected by conductor 16 to receive input voltage Vin−. (Note that input transistors Q0 and Q1 are analogous to input transistors Q0 and Q1 in Prior Art
Input stage 1-1 also includes a maximum voltage selector circuit 22 that includes voltage selector JFETs P1 and P2, which are referred to simply as “voltage selector transistors”. Voltage selector circuit 22 also includes resistors R1 and R2. The second terminal of voltage selector transistor P1 is coupled by resistor R1 to conductor 19, and the second terminal of voltage selector transistor P2 is coupled by resistor R2 to conductor 19. Conductor 19 is connected to the gates of voltage selector transistors P1 and P2 and also to the gate of pass transistor P3. (It should be understood that each current-carrying electrode of a field effect transistor may function either as a source or a drain, depending on which electrode is at a higher voltage. If at any particular time one current-carrying electrode is functioning as the source of the field effect transistor, the other electrode is functioning as the drain, or vice versa.) A clamping circuit 14 includes maximum voltage selector circuit 22 and level shift transistors N1 and N2. Pass transistor P3 also may be considered to be a part of clamping circuit 14. (In some cases it might be possible to use a depletion mode MOSFET (metal oxide semiconductor field effect transistor) as pass transistor P3. In some cases, it might also be practical to use depletion mode MOSFETs as voltage selector transistors. In some cases it might also be practical to use JFETs or depletion mode MOSFETs as resistors R1 and R2.)
The sources of N-channel level shift transistors N1 and N2 in
Maximum voltage selector circuit 22 operates to control the gate bias voltage of pass transistor P3. In a “balanced” mode of operation Vin+ and Vin− are approximately equal, and in a “unbalanced” mode of operation the maximum differential input voltage VD(max)=Vin+−Vin− is greater than approximately 2 volts.
Balanced Mode Operation for Vin+≈Vin−
Still referring to
Specifically, Vin+ is applied to the gate of level shift transistor N1. With the current I2 biasing level shift transistor N1, its source voltage is approximately a VBE voltage more positive than its gate voltage, so the voltage of conductor 20 connected between the source of level shift transistor N1 and the source of voltage selector transistor P1 is at approximately the same voltage as the emitter of input transistor Q0. (The gate-source voltage of level shift transistor N1 (or N2) depends on its scaling (i.e., its channel width to channel length ratio W/L) and the amount of current flowing in that device. An appropriate choice of device scaling is required to obtain a value of the gate-source voltage of level shift transistor N1 (or N2) of approximately one VGS voltage with current I2 (or I3) flowing through it. Similarly, Vin− is applied to the gate of level shift transistor N2. With the current I3 biasing level shift transistor N2, its source voltage is also approximately a VBE more positive than its gate voltage, so the voltage of conductor 21 between the source of level shift transistor N2 and the source of voltage selector transistor P2 is at the same voltage as the emitter of input transistor Q1.
Thus, during balanced-input operation essentially the same voltages are present on the sources of level shift transistors N1 and N2 and the emitters of input transistors Q0 and Q1. Voltage selector transistors P1 and P2 are in their triode regions and therefore appear as equal resistances in series with resistors R1 and R2, which also are equal. The average voltage value on conductor 19 biases the gate of pass transistor P3 it at approximately the same voltage as the voltages on its drain and source, and that causes it to operate in its triode region so it appears as a resistor connected between the emitters of input transistors Q0 and Q1. Input stage 1-1 therefore averages the source voltages of level shift transistors N1 and N2 and applies that average voltage, minus the source-gate voltage of voltage selector transistors P1 and P2, to the gate of pass transistor P3 by means of conductor 19 when input voltages Vin+ and Vin− are equal, i.e., balanced.
Unbalanced Mode Operation for Vin+−Vin−>2 Volts
Referring to
Since voltage selector transistor P1 is a P-channel device, the resulting voltage between its P-type drain and N-type gate may cause that PN junction to become forward biased with respect to the N-type gate of transistor P1. This results in a diode-type current flow from the source to the gate of voltage selector transistor P1. Conductor 19 is connected to the gate of voltage selector transistor P1 and also to the gate of pass transistor P3, so there is a diode-type VBE voltage drop of about 0.3 to 0.4 volts between the source of level shift transistor N1 and the gate of pass transistor P3. The diode-type current flowing through the forward-biased source-gate junction of voltage selector transistor P1 also flows through voltage selector transistor P2 and resistor R2. (In fact, preferred operation is to not forward bias this junction of level shift transistor N1 even for a maximum value of the current I2 plus the drain current of maximum selector transistor P2. The drain current of selector transistor P2 should always be less than the current I3 so that there is always current in level shift transistor N2.)
In any case, the resulting voltage developed across resistor R2 applies a gate-source voltage to voltage selector transistor P2. The current through resistor R2 increases until an equilibrium is reached wherein the gate-source voltage of transistor P2 suitably limits the amount of current through voltage selector transistor P1, which is operating as a forward-biased diode. The magnitude of the current through voltage selector transistor P2 should be less than either of currents I2 or I3 to ensure flow of current through level shift transistor N2 so that its source voltage is still more positive than its gate voltage. Since voltage selector transistor P1 operates as a forward-biased diode, it keeps the gate voltage of pass transistor P3 near Vin+.
The voltage V20 on conductor 20, which is connected to the source of level shift transistor N1, is equal to Vin+ plus the VGS(N1) voltage of level shift transistor N1. The gate-source voltage of level shift transistor N1 would not forward bias that junction, and would be slightly less in magnitude than in the balanced mode of operation. That is, in the unbalanced mode of operation, the source of level shift transistor N1 might be 50-100 millivolts lower than in the balanced mode case but not enough lower to forward bias the gate-source junction. The voltage V19 on conductor 19, i.e., on the gate of voltage selector transistor P1, is equal to V20 minus the VBE(P1) voltage drop across the forward-biased source-gate junction of voltage selector transistor P1. The voltage V11A on conductor 11A, i.e., on the emitter of input transistor Q0, is equal to V19 minus the gate-source voltage of pass transistor P3, which is somewhat less than its pinch-off voltage VP(P3). That causes input transistor Q0 to turn off as Vin+ continues to increase, thereby causing all of the current I0 to flow through pass transistor P3. This operation limits the reverse bias voltage across the emitter-base junction of input transistor Q0 and prevents hot electron injection from occurring in it. The operation and effect are entirely similar for the case in which Vin− is substantially greater than Vin+. Note that the foregoing analysis is subsequently set forth in more detail, with reference to
Input follower circuit 30 includes a NPN follower transistor Q3 having its base connected by conductor 15 to receive Vin+ and also connected to the cathode of a diode D0. The collector of follower transistor Q3 is connected to VCC and its emitter is connected by conductor 23 to the gate of level shift transistor N1, the anode of diode D0, and one terminal of a level shift resistor R0 having its other terminal connected by conductor 26 to the base of PNP input transistor Q0, one terminal of current source I1, and to the anode of a diode D4. The cathode of diode D4 is connected to the anode of a diode D1, the cathode of which is connected to conductor 11A. Similarly, input follower circuit 31 includes a NPN follower transistor Q4 having its base connected by conductor 16 to receive Vin− and also connected to the cathode of a diode D7. The collector of follower transistor Q4 is connected to VCC and its emitter is connected by conductor 24 to the gate of level shift transistor N2, the anode of diode D7, and one terminal of a level shift resistor R3 having its other terminal connected by conductor 27 to the base of PNP input transistor Q1, one terminal of current source I4, and to the anode of a diode D5. The cathode of diode D5 is connected to the anode of a diode D6, the cathode of which is connected to conductor 11B.
Thus, differential input signal Vin+−Vin− is applied to an emitter follower stage 30,31 which drives a differential input transistor pair Q0,Q1. Differential clamping circuitry 14 includes level shift transistors N1 and N2, voltage selector transistors P1 and P2, level shift resistors R1 and R2, and pass transistor P3 and operates to clamp or limit reverse bias of the base-emitter junctions of input transistors Q0 and Q1. The emitter-base junctions of differential transistor pair Q0,Q1 are protected by differential clamping circuitry 14, which operates to clamp the VEBO voltage of the input transistor Q0 or Q1 which is cut off to approximately 1 volt or less. The clamping circuitry 14 operates properly even when the input signal Vin+ or Vin− swings to a level equal to one VBE voltage above the upper supply rail voltage VCC.
As previously mentioned, the lifetime of either of input transistors Q0 and Q1 may be reduced to as little as a few minutes if its VEBO reverse breakdown voltage is greater than 1.5 volts and thereby causes hot carrier injection to occur in the reverse-biased emitter-base junction. In PNP transistors, the emitter-base breakdown voltage VEBO typically is greater than 1.2 volts, and is greater than approximately 2.2 volts in NPN transistors. Input stage 1-2 may be designed to have a safe region of operation which keeps VEBO below 1.2 volts so that input stage 1-2 is suitable for use in input stages having both NPN and PNP transistors.
An operating point analysis of JFET clamping circuitry 14 shown in
V23=VG(N1)=Vin+−VBE(Q3)
and
V24=VG(N2)=Vin−−VBE(Q4),
where V23 and V24 are the voltages on conductors 23 and 24, respectively.
Since level shift transistors N1 and N2 should always be in an active ON condition, the current through maximum voltage selector transistors P1 and P2 must satisfy the expression
IMVS−INB>0
where, IMVS is equal to the current through maximum voltage selector transistors P1 and P2 and INB is equal to the tail current I2 for level shift transistor N1 and also is equal to tail current I3 for level shift transistor N2. This is to ensure that the voltage V20 at the source of level shift transistor N1 and the voltage V21 at the source terminal of level shift transistor N2 are given by the expressions
V20=VS(N1)=Vin++VBE(Q3)−VGS(N1)
and
V21=VS(N2)=Vin−−VBE(Q4)−VGS(N2),
respectively.
Therefore, assuming that Vin+ is greater than Vin−, maximum voltage selector circuit 22 causes the voltage at the gate of pass transistor P3 to be
V19=VG(P3)=Vin+−VBE(Q3)ABS{VGS(N1)}−VSG(P1),
where V19 is the voltage on conductor 19, VBE(P1) is the voltage drop across the forward-biased source-drain junction of voltage selector transistor P1 and ABS{VGS(N1)} is the absolute value of VGS(N1).
Pass transistor P3 is sized so as to provide a suitable amount of degeneration in emitter-coupled input transistors Q0 and Q1. The final voltage at the emitter of the inactive (i.e., OFF or cut-off) bipolar transistor Q0 therefore is determined according to
VE(Q0)=Vin+−VBE(Q3)−VGS(N1)−VSG(P1)−VGS(P3),
where VGS(P3) is always less than the pinch-off voltage VP(P3).
A similar equation provides the final voltage at the emitter of input transistor Q1. Accordingly, VEBO can be calculated according to the expression
VEBO(Q0 or Q1)=I×R(R0 or R3)+VGS(N1 or N2)−VSG(P1 or P2)−VGS(P3).
(Note that the voltage of transistor Q3 or Q4 does not factor into the VBE of Q0 or Q1, since the top terminals of resistors R0 and R1 as shown in
Using worst case values for the parameters in the foregoing equation for a particular wafer fabrication process, the maximum value of VEBO is 1.2 volts. Thus, the emitter-base junctions of the input pair transistors Q0, Q1 are protected from reverse voltage breakdown and associated hot carrier injection.
In order to limit the saturation current of the P-channel JFET “diodes” P1 and P2 in maximum voltage selector circuit 22 to a low value, e.g. less than 1 microampere in one example, series level shift resistors R1 and R2 with resistances of approximately 800 kilohms are used in the diode-connected loops. (The term “diode connected loops” refers to the connection of gate of voltage selector transistor P2 to its source through resistor R2. Current in maximum voltage selector circuit 22 is limited by the fact that the voltage drop across resistor R2 results in a VGS voltage on maximum voltage selector transistor P2 to reduce current flow therein. Resistor R2 results in lower current than would otherwise flow if the gate and source of voltage selector transistor P2 were directly connected together. Level shift resistors R0 and R3 serve two purposes, including (1) providing additional positive level shift relative to base of Q0 or Q1 to reduce the amount of reverse bias on transistor Q0 or Q1 during unbalanced operation, and (2) allowing for voltage compliance of current sources I0 and I5 when the base of transistor Q3 and/or Q4 are higher than VCC. (For Vin+=VCC+VBE, VE(Q) will be Vin+−VBE(Q3)−I1*R0+VBE(Q)=VCC−I1*R0, which allows a voltage of I1*R0 within which current source I0 can operate.
It has been found that the differential clamping circuitry 14 does not respond satisfactorily to fast transients in differential mode or in common mode voltages applied to the input of input stage 1-2 of
Diodes D0 and D7 are connected as clamps across the emitter-base junctions of follower transistors Q3 and Q4 to prevent reverse biasing their emitter-base junctions during fast signal transitions of Vin+ and Vin−. Diodes D1, D4, D5, and D6 serve as clamps across input transistors Q0 and Q1 for the same reason. After a very fast input signal transient has settled, current source I1 continues to keep current flowing in emitter follower transistor Q3 so it remains ON. Similarly, current source I4 continues to keep current flowing in emitter follower transistor Q4 so it also remains ON. This is advantageous because without diodes D0 and D7, it is possible to substantially reverse bias the emitter-base junctions of Q3 and Q4 and thereby interrupts their operation during a very high speed input signal transient.
The currents I1 and I4 flow through resistors R0 and R1 and generate voltage shifts of a few hundred millivolts across each. The amount of this voltage shift is based on the characteristics of level shift transistors N1 and N2 as well the reverse bias of the emitter-base voltages that, in the case of a worst case process variation of the pinch-off voltage VP of pass transistor P3, would occur on input transistors Q0 and Q1 for very large magnitudes of the differential input voltage Vin+−Vin− if the foregoing voltage shifts are not provided. The voltage shifts across resistors R0 and R1 reduce the amount of reverse bias on the emitter-base junctions of input transistors Q0 and Q1.
A circuit similar to the one shown in
In
One terminal of pass transistor N3 is connected by conductor 11A to the emitter of input transistor Q0 and to one terminal of current source I0, the other terminal of which is connected to VSS. The collector of input transistor Q0 is connected to Vout−. The other terminal of pass transistor N3 is connected by conductor 11B to the emitter of input transistor Q1 and to one terminal of current source I5, the other terminal of which is connected to VSS. The collector of input transistor Q1 is connected to Vout+. The gate of pass transistor N3 is connected by conductor 19 to one terminal of each of voltage selector transistors P1 and P2. The gate of voltage selector transistor P1 is connected by conductor 20 to one terminal of resistor R1, the other terminal of which is connected to the remaining terminal of voltage selector transistor P1. Similarly, the gate of voltage selector transistor P2 is connected by conductor 21 to one terminal of resistor R2, the other terminal of which is connected to the remaining terminal of voltage selector transistor P2.
Input follower circuit 30A includes a PNP follower transistor Q3 having its base connected by conductor 15 to receive Vin+ and also connected to the anode of a diode D0. The collector of follower transistor Q3 is connected to VSS and its emitter is connected by conductor 23 to the gate of level shift transistor Px, the cathode of diode D0, and one terminal of a level shift resistor R0 having its other terminal connected by conductor 26 to the base of NPN input transistor Q0, one terminal of current source I1, and to the cathode of a diode D4. The anode of diode D4 is connected to the cathode of a diode D1, the anode of which is connected to conductor 11A. Similarly, input follower circuit 31A includes a PNP follower transistor Q4 having its base connected by conductor 16 to receive Vin− and also connected to the anode of a diode D7. The collector of follower transistor Q4 is connected to VSS and its emitter is connected by conductor 24 to the gate of P-channel level shift transistor Py, the cathode of diode D7, and one terminal of a level shift resistor R3 having its other terminal connected by conductor 27 to the base of NPN input transistor Q1, one terminal of current source I4, and to the cathode of a diode D5. The anode of diode D5 is connected to the cathode of a diode D6, the anode of which is connected to conductor 11B.
Thus, differential input signal Vin+−Vin− is applied to an emitter follower stage 30A,31A which drives a differential input transistor pair Q0,Q1. Differential clamping circuitry 14 includes level shift transistors Px and Py, voltage selector transistors P1 and P2, level shift resistors R1 and R2, and pass transistor N3 and operates to clamp or limit reverse bias of the base-emitter junctions of input transistors Q0 and Q1. The emitter-base junctions of differential transistor pair Q0,Q1 are protected by differential clamping circuitry 14, which operates to clamp the VEBO voltage of the input transistor Q0 or Q1 which is cut off to approximately 1 volt or less. The clamping circuitry 14 operates properly even when the input signal Vin+ or Vin− swings to a level equal to one VBE voltage above the upper supply rail voltage VCC.
Note that the maximum voltage selector circuit 22 shown in
In the case of a maximum voltage selector circuit, for example, as shown in
The described embodiments of the invention use simple circuitry composed of JFETs, resistors, and bipolar transistors to clamp the base-emitter junctions of the input transistors so as to prevent hot carrier injection without degrading the normal performance of the differentially coupled input transistors of an input stage. The described embodiments operate as efficiently for small input differential signals as for large input differential signals. Furthermore, the technique of the invention can be used for CMOS and JFET differential pair input transistors as well as for bipolar differential pair input transistors without substantial modification to the basic circuitry described herein.
It should be understood that the differential input circuits described herein can be readily operated as single-ended input circuits by simply connecting one of the inputs to a reference voltage and connecting the other input to receive a single-ended input signal.
While the invention has been described with reference to several particular embodiments thereof, those skilled in the art will be able to make various modifications to the described embodiments of the invention without departing from its true spirit and scope. It is intended that all elements or steps which are insubstantially different from those recited in the claims but perform substantially the same functions, respectively, in substantially the same way to achieve the same result as what is claimed are within the scope of the invention. For example, although the field effect transistors in the described embodiments are JFETs, it may be practical in some cases to implement some of them as depletion mode MOSFETs.
Doorenbos, Jerry L., Udayashankar, Sudarshan
Patent | Priority | Assignee | Title |
10873331, | Aug 25 2017 | RichWave Technology Corp. | Clamp logic circuit |
8901967, | Dec 03 2012 | Fuji Electric Co., Ltd. | Comparator |
Patent | Priority | Assignee | Title |
6271688, | Jul 17 1999 | STMICROELECTRONICS S R L | MOS transconductor with broad trimming range |
7339402, | Feb 13 2006 | Texas Instruments Incorporated | Differential amplifier with over-voltage protection and method |
7554364, | Feb 13 2006 | Texas Instruments Incorporated | High-voltage operational amplifier input stage and method |
Executed on | Assignor | Assignee | Conveyance | Frame | Reel | Doc |
Jul 22 2010 | DOORENBOS, JERRY L | Texas Instruments Incorporated | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 024801 | /0958 | |
Jul 22 2010 | UDAYASHANKAR, SUDARSHAN | Texas Instruments Incorporated | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 024801 | /0958 | |
Jul 27 2010 | Texas Instruments Incorporated | (assignment on the face of the patent) | / |
Date | Maintenance Fee Events |
Sep 24 2015 | M1551: Payment of Maintenance Fee, 4th Year, Large Entity. |
Sep 16 2019 | M1552: Payment of Maintenance Fee, 8th Year, Large Entity. |
Sep 20 2023 | M1553: Payment of Maintenance Fee, 12th Year, Large Entity. |
Date | Maintenance Schedule |
Apr 24 2015 | 4 years fee payment window open |
Oct 24 2015 | 6 months grace period start (w surcharge) |
Apr 24 2016 | patent expiry (for year 4) |
Apr 24 2018 | 2 years to revive unintentionally abandoned end. (for year 4) |
Apr 24 2019 | 8 years fee payment window open |
Oct 24 2019 | 6 months grace period start (w surcharge) |
Apr 24 2020 | patent expiry (for year 8) |
Apr 24 2022 | 2 years to revive unintentionally abandoned end. (for year 8) |
Apr 24 2023 | 12 years fee payment window open |
Oct 24 2023 | 6 months grace period start (w surcharge) |
Apr 24 2024 | patent expiry (for year 12) |
Apr 24 2026 | 2 years to revive unintentionally abandoned end. (for year 12) |